Control of pattern formation in a single feedback system by photonic lattices

Figure 6: (A, B) FDTD simulations of FRET rate enhancement (left column), donor rate enhancement (middle column) and resulting FRET efficiency (right column) as a function of

After describing the optimal solution of a model tracking problem, we propose a feedback control structure in order to take into account a possible modeling error.. We present

In summary, we have obtained in the figure-of-eight double-clad fiber laser a variety of soliton patterns involing a large number of pulses.. Some of these patterns were

We will show that the homogeneous equilibrium stable in the case of the usual logistic equation can become unstable in the case of nonlocal consumption of resources.. It is a

irom the field direction due to the elastic coupling to the surface. Since in thin cells the thickness d is of the order of the magnetic coherence length I, these disto~ions of

By analogy it was concluded [4] that problems of pattern recognition could be solved by application of similar principles, if they were.. realized appropriately on

However, even for 2D patterns, the spatial variability of ripples formed by a monochromatic gravity wave of high quality in a flume suggests that statistics on distributions of

First, we mine every single size-2 weighted path (with one edge) that is condensed regarding the set of size-2 (only) weighted patterns. Those triplets match frequent triadic